376864b3f79917a82fc6482592cc2db2.ppt
- Количество слайдов: 93
Drops on patterned surfaces Halim Kusumaatmaja Alexandre Dupuis Julia Yeomans
Summary The model Chemically patterned surfaces Spreading on stripes Hysteresis Superhydrophobic surfaces Introduction Hysteresis Transitions between states Dynamics
Equations Navier-Stokes equations of motion continuity Navier-Stokes No-slip boundary conditions on the velocity
Equilibrium free energy bulk term interface free energy surface term Van der Waals controls surface tension controls contact angle
Controlling the contact angle Surface free energy Minimising the free energy leads to: Boundary condition on the Euler-Lagrange equation A relation between the contact angle and the surface field
Summary The model Chemically patterned surfaces Spreading on stripes Hysteresis Superhydrophobic surfaces Introduction Hysteresis Transitions between states Dynamics
Chemically striped surfaces: drop spreading
Experiments (J. Léopoldès and D. Bucknall) 64 o / 5 o
LB simulations on substrate 4 • Two final (meta-)stable state observed depending on the point of impact. • Dynamics of the drop formation traced. • Quantitative agreement with experiment. Simulation vs experiments Evolution of the contact line
Impact near the centre of the lyophobic stripe
Impact near a lyophilic stripe
LB simulations on substrate 4 • Two final (meta-)stable state observed depending on the point of impact. • Dynamics of the drop formation traced. • Quantitative agreement with experiment. Simulation vs experiments Evolution of the contact line
80 o /90 o
Two wide stripes: 110 o /130 o hydrophilic hydrophobic hydrophilic
80 o /90 o
Characteristic spreading velocity A. Wagner and A. Briant
Summary The model Chemically patterned surfaces Spreading on stripes Hysteresis Superhydrophobic surfaces Introduction Hysteresis Transitions between states Dynamics
Hysteresis
Hysteresis
Hysteresis
Hysteresis
Hysteresis
Hysteresis
Hysteresis
Hysteresis
Hysteresis
Hysteresis slips at angle advancing
Hysteresis pinned until
Hysteresis pinned until
Hysteresis slips smoothly across hydrophobic stripe
Hysteresis slips smoothly across hydrophobic stripe
Hysteresis jumps back to
Hysteresis advancing stick slip jump (slip)
Hysteresis advancing stick slip jump (slip) receding stick (slip) jump slip
(Hysteresis) loop a contact angle a volume advancing contact angle receding contact angle a
(Hysteresis) loop slip contact angle stick volume advancing contact angle receding contact angle jump
Hysteresis: 3 dimensions A. squares 60 o background 110 o B. squares 110 o background 60 o
Hysteresis: 3 dimensions A squares hydrophilic B squares hydrophobic
Hysteresis: 3 dimensions macroscopic contact angle versus volume A stick B jump
Hysteresis: 3 dimensions macroscopic contact angle versus volume A B 94 o 92 o 110/60
Hysteresis on chemically patterned surfaces 1. Slip, stick, jump behaviour, but jumps at different volumes in different directions (but can be correlated) 2. Contact angle hysteresis different in different directions 3. Advancing angle (92 o) bounded by qmax (110 o) Receding angle (80 o) bounded by qmin (60 o) 4. Free energy balance between surface / drop interactions and interface distortions determines the hysteresis
Summary The model Chemically patterned surfaces Spreading on stripes Hysteresis Superhydrophobic surfaces Introduction Hysteresis Transitions between states Dynamics
Superhydrophobic surfaces
Superhydrophobic surfaces
Two drop states suspended drop collapsed drop He et al. , Langmuir, 19, 4999, 2003
Suspended and collapsed drops Suspended, q~160 o Homogeneous substrate, qeq=110 o Collapsed, q~140 o
Hysteresis: suspended state 180 o
Hysteresis: suspended state advancing receding Suspended drop Advancing contact angle 180 o: pinned on outside of posts Receding contact angle : pinned on outside of posts
Hysteresis: collapsed state receding Collapsed drop Advancing contact angle 180 o: pinned on outside of posts Receding contact angle -90 o: pinned on outside AND inside of posts
Hysteresis: three dimensions 2 D Suspended drop: advancing angle 180 o receding angle qe Collapsed drop: advancing angle 180 o receding angle qe-90 o 3 D
Hysteresis: three dimensions 2 D Suspended drop: advancing angle 180 o receding angle qe 3 D 180 o > qe Free energy barrier very small Collapsed drop: advancing angle 180 o receding angle qe-90 o ~180 o > qe-90 o
Hysteresis on superhydrophobic surfaces 1. Advancing contact angles are close to 180 o 2. Hysteresis smaller for suspended than collapsed drop High receding contact angle -- weak adhesion Small contact angle hysteresis – slides easily? ? 3. Free energy balance between drop -- surface interactions and interface distortion determines the hysteresis ? ? Forced hysteresis ? ? Changing relative length scales ? ? Relation between hysteresis and easy run off
Summary The model Chemically patterned surfaces Spreading on stripes Hysteresis Superhydrophobic surfaces Introduction Hysteresis Transitions between states Dynamics
Drop collapse: Mathilde Reyssat and David Quere 200 m
Drop collapse: simulations
1. Curvature driven collapse : short posts 2. Free energy driven collapse : long posts
Drop collapse: short posts
Drop collapse: short posts
Drop collapse: short posts Drop collapse: simulations Mathilde Reyssat and David Quere
Drop collapse: shallow posts
Drop collapse: long posts
Drop collapse: long posts qe Deep posts: contact angle reaches qe on side of posts
Variation of free energy with post height q>qe q
Drop collapse: two dimensions
Drop position with decreasing contact angle
Collapse on superhydrophobic surfaces Shallow posts: curvature driven collapse Deep posts: 2 dimensions – free energy driven collapse Deep posts: 3 dimensions – is collapse possible ? ?
Summary The model Chemically patterned surfaces Spreading on stripes Hysteresis Superhydrophobic surfaces Introduction Hysteresis Transitions between states Dynamics
With thanks to Alexandre Dupuis Halim Kusumaatmaja
Drop velocity: suspended drop Droplet velocity Drop velocity
Drop velocity: collapsed drop Dynamics of collapsed droplets Drop velocity
Summary The model Chemically patterned surfaces Spreading on stripes Hysteresis Superhydrophobic surfaces Introduction Hysteresis Transitions between states Dynamics
With thanks to Alexandre Dupuis Halim Kusumaatmaja
Chemically striped surfaces: drop motion
Two wide stripes: 110 o /130 o hydrophilic hydrophobic hydrophilic
80 o /90 o
60 o /110 o
Base radius as a function of time
Controlling the contact angle Surface free energy Minimising the free energy leads to: Boundary condition on the Euler-Lagrange equation A relation between the contact angle and the surface field
Mathilde Callies and David Quere 2006


